Thermistors Thermistors A thermistor is a thermally sensitive semiconductor whose resistance varies with temperature Semiconductor materials: Typically oxides of Nickel Copper Uranium Typically have a large negative temperature coefficient (NTC) Resistance function is non-linear Static sensitivity is much larger than for RTDs Image source: http://image.made-in-china.com/2f1j00tvaEnRwKaGpC/Power-NTC-Thermistors-MF72-.jpg Manganese Cobalt Iron Resistance decreases with increasing temperature Dr. Christopher M. Godfrey University of North Carolina at Asheville ATMS 320 ATMS 320 How are thermistors made? Cut the wires to shape A dollop of slurry made of mixed metal oxides and a suitable binder is dropped onto platinum alloy wires Dollop of thermistor material The wires are cut to shape depending on the use of the device Opposite Cut Double Adjacent Cut Uncut strand of beads Surface tension forms an ellipsoidal shape The metals are heated to form an electrical contact with the wires Adjacent Cut ATMS 320 Thermistor Coatings Glass Probe ATMS 320 Thermistor Transfer Equation ATMS 320 The thermistor is usually coated with glass and/or another protective covering to seal the thermistor and provide some strain relief There are several possible transfer equations for different thermistors In all cases, the resistance of a thermistor is a function of the absolute temperature ATMS 320 1 Steinhart-Hart Equation Studies have shown that a good relationship for a thermistor exists between ln(RT) and a polynomial of 1/T ln RT b0 Steinhart-Hart Equation a a RT exp a0 1 33 T T b1 b2 ... T T2 RT = Resistance at T (in K) Empirical tests have shown that only three terms are required for accurate measurements: This is one version of the Steinhart-Hart equation Requires many calibration coefficients Very nonlinear Nonlinearities can be corrected with analog conditioning circuits such as bridge circuits or by using microprocessors ATMS 320 Thermistor Transfer Equation ATMS 320 Thermistor Linearizing Circuit a a RT exp a0 1 33 T T Static sensitivity is not constant, but decreases with increasing temperature Amplification would result in HUGE values for low temperatures An almost linear circuit with two thermistors ATMS 320 Thermistor Linearizing Circuit ATMS 320 Thermistor Advantages High resistance (1 k to 100 k) Highly non-linear RT vs. T relationships ATMS 320 Mostly negative temperature coefficients (NTC) from metal oxides, but positive temperature coefficient (PTC) models are available from barium and strontium titanate mixtures Can be linearized Small physical size The voltage output (left) and residual nonlinearity (right) from the linearizing circuit with properties given in your textbook (p. 75) Eliminates problems with resistance in lead wires Fast response time Not as small as thermocouples ATMS 320 2 Thermistor Advantages Easy to manufacture in bulk Wide temperature range Very high sensitivity and resolution Thermistor Disadvantages Lower cost than RTDs Up to 1000 times more sensitive than RTDs Can withstand shock and vibration Accurate Image source: http://www.advindsys.com/Products/Thermistors.htm The nonlinear response requires extra circuitry Limited range of linear response with this additional circuitry Narrow “linear” operating range for a single sensor The glass can break if mishandled Requires an excitation current High resistance leads to self-heating errors (more so than RTDs) Less stable than RTDs ATMS 320 ATMS 320 Comparison of Resistance Thermometers SS Comparison of Resistance Thermometers dRT dT Resistance Temperature Detector Source: http://www.designinfo.com/cornerstone/ref/negtemp.html ATMS 320 Resistance Thermometers: A Summary The electrical resistance of various materials changes in a reproducible way when subjected to temperature variations. An RTD (resistance temperature detector) is a precision temperature-sensing device that utilizes metal conductors (typically a fine platinum wire winding or a thin metallic layer applied to a substrate) and has a positive coefficient of resistance. That is, as T increases, resistance increases almost linearly. These are called positive temperature coefficient devices (PTC). Thermistors are made from semiconductor materials that have a large negative coefficient of resistance. That is, as T increases, resistance decreases. These are called negative temperature coefficient (NTC) thermistors. ATMS 320 ATMS 320 Other types of temperature sensors: Capacitive Sensors C K 0 A d Once we fix A and d, the only variable that can change is the dielectric constant, K, which changes with temperature ATMS 320 3 Other types of temperature sensors: Other types of temperature sensors: Integrated Circuit (IC) Thermometer Infrared Camera Used in automotive applications and cheap weather sensors Sensor and signal conditioning circuits all located on a single integrated circuit Accuracy is ~0.5°C Low cost ATMS 320 ATMS 320 Other types of temperature sensors: Sensor Choice Infrared Thermocouple Receives heat energy from object and converts to electrical potential Unpowered Low cost Non-invasive Fast response time ATMS 320 How do we decide which type of sensor to use? Usually depends on your application Cost Size Additional circuitry Accuracy Response time We can also make a decision by determining which sensor requires the least amount of gain ATMS 320 Figure of Merit Assuming all other things are equal, look at the gain: Figure of merit = log10 G 1 We want the smallest gain possible High gain amplifier amplifies noise and the signal and is more expensive In this example, the thermistor is the best bet, but this may not be the case for your application! ATMS 320 4